US2572216A - Signal receiving system - Google Patents

Description

Oct 23, 1951 E. R. TAYLOR SIGNAL RECEIVING SYSTEM 2 SHEETS-SHEET l Filed April I, 1944 kbmt /N VEN TOR E. Fr. TA YL OR Oct. 23, 1951 E, R TAYLOR SIGNAL RECEIVING SYSTEM 2 SHEETS-SHEET 2 Filed April l, 1944 Patented Oct. 23, `1951 SIGNAL RECEIVING SYSTEM Edmund R. Taylor, Pelham Manor, N. Y., assignor to Bell Telephone Laboratories, Incorporated,` New York, N. Y., a corporation of New York Application April 1,1944, Serial No. 529,092

" 7 Claims.

1 e j This invention relates to scanning systems an more particularly to systems in which a selective means cyclically scans a Wave frequency range r other subject and selects in succession wave effects of diiferent frequencies that appear in the frequency range, or other effects according to the nature of the subject, and in which the successively selected eiects are individually oscila loscopically displayed or otherwise utilized.

I A broad object of this invention is to provide an improved frequency scanning system of increased accuracy, sensitivity and flexibility capable of dependable operation over a Wide frequency range.

A further object is to/reduce the range of frequency variation required of the beating oscillator in the heterodyne type of frequency range scanner.

A further object is to eliminate the practical difficulty of obtaining wide monitoring frequency ranges without resort to high operating frequencies.

` A more specific object is to offset or neutralize the undesirable effects that changes in temperature and other operating conditions have on the operation of a scanning system.

' In accordance with the present invention, as embodied in a frequency scanning system, a plurality of frequency scanners are employed in tandem relation, the first scanner being cyclically operative over the frequency range of interest and each other scanner being connected to scan the wave output of the preceding scanner. In accordance with a feature of the invention the first of the tandemscanners is assigned a relatively broad frequency selective characteristic and succeeding scanners have progressively narrower frequency selective characteristics. Another feature provides for maintaining the band of waves delivered by each scanner at a fixed frequency position whereby the succeeding scanner is required to operate over only a limited fixed frequency range. In accordance with still other features the eiect that changes in temperature and other operating conditions have on the operation of one frequency scanner is oiiset or neutralized by the effects such changes have on another of the scanners. As the expression is used herein, scanning denotes a process in which the elements constituting the total subject are, repeatedly and continually, selected successively in a systematic manner. "Frequency scanning denotes scanning in which the elements are sel'ected according to frequency, or in other lWords it signifies continuallyrepeated successive selection of the different components of a wavefre-;

quency range. v The nature of the present inventionA andii various features, objects and advantages vvill'ap` pear more fully from a consideration of the folv lowing description of the embodiments 'illustrated-1 inthe accompanying drawings.l In the drawingsz" Fig. 1 illustrates a so-called panoramic radio receiving system for monitoring a predeterminedrange of radio frequencies and indicating oscille--A scopically the frequencies of the signals appea`r` ing in that range; y f Fig. 2 illustrates diagrammatically certain'feajA tures of the design and operation of the Fig. '1" system; and Figs. 3 and 4 illustrate other embodiments. of the invention. a Referring more particularly now to Fig. 1, the system illustrated therein comprises a radio lreceiving antenna I and a radio frequency amplii fier 2 through which all received waves lying within the frequency range of interest areap plied to the input of a frequency scanner 3. The frequency range of interest may be for specificv example the radio broadcast band. Scanner 3 comprises a modulator A to which the received band is applied and a variable frequency oscil-f lator 5 for supplying beating oscillations con,-l currently to the modulator 4. Inthe output 'of modulator 4 the applied frequency band appears as a sideband, translated in frequencyr more or less. according to the operating frequency of oscillator 5. The sideband, and vit will be sumed that it is an upper sideband, is applied to a band-pass lter 6 which has a relatively broadfrequency selective characteristic. The width of band passed by filter S'may be for specific exiample one-quarter of the width of the applied.V sideband. The operating frequency of oscillator 5 is variedcyclically between predetermined limits such that at the output of modulator 4 the sideband pro`4 gresses during each cycle from an initial or upper frequency position PI to a lower frequency position P2 and returns instantly to its initial posi'f tion PI for the beginning of the next cycle. TheY limits are so chosen with reference to the pass frequency of filter 6 that with the sideband in the position PI the lower quarter of the sideband is passed by the lter and with the sideband in position P2, the upper quarter is passed by the filter. These relations are indicated diagrammatically in' Fig. 2. In purpose and effect the filter 6 and the frequency scanner 3 of which itis a part repeateda 1y traverse the frequency range of interest and at;

each point in the traverse select all of the signals lying within a fractional part of the frequency range. The wave output of scanner 3 and filter 6 is of continually changing composition but is confined to the pass frequency range of iilter S.

The output of the scanner 3 is connected to the input of a second frequency scanner I. |The latter comprisesa modulator 8, anassociated beating oscillator 9 and a band-pass filter IIJ-connected to the output of the modulator. The operating frequency of oscillator 9 is varied in the same manner as that of oscillator and between frequency limits such that one of the sidebands derived from the band of waves. received from the scanner 3 is swept repeatedly across the pass frequency of lter I0. The extremepositions P3 and P4 of the sideband, assuming again an upper sideband, are represented in Fig. 2 in relation to the pass-band of filter I Il. The latter is made narrow enough to discriminate between and selectively transmitthe'severalradio signals that may be encountered in the applied sideband.v

*The cyclicalv operation of the two frequency scanners 3 and I may be so synchronized in a manner to be described that While scanner 3 progresses from the low frequency end to the high frequency end Vof the radioV frequency range, scanner 'I simultaneously progresses from the low end to the highend of the pass-band of filter 5. In `such case scanner 'I ineffect cyclically traverses the radio frequency range to be monitored and transmits in succession the signals of different frequenciesthat are successively encountered therein. At the output terminals of-filter I3 each signal appears momentarily, once during each scanning cycle, and at the same relative point in each cycle.

The output circuity of frequency scanner 1 is connected through a `rectifier II to the deflecting plates I3 of afcathode ray 'tube I2. Rectifier II serves to convert each momentarily applied signal wave into a unidirectional voltage that is more or less proportional to the intensity of the signal. Deilecting plates .I3 :are so oriented that the cathode-ray and also `the luminous spot produced by the ray on luminescent screen I5 are deflected vertically upward VWhenever a signal-produced unidirectional voltage is received from rectifier I I.. .The position of the luminous spot along ahorizontal reference axis, or frequency scale, on the screen I5-is simultaneously controlled by deflecting plates I4 and a control voltage applied thereto from sweep circuit 20. The latter produces a periodic voltage wave of such shape and phase that the spot moves along the horizontal frequency scale in synchronism with the relative progression of scanner 'I across the radio -frequency range. Each pointV along the frequency scale can therefore be identified with a particular. radio frequency. During each scanning cycle, then, the luminousfspot moves along the frequencyscale and Whenever a signal is encountered by the scanning system it is deflected vertically upWardleavinga vertical luminous line the position of which identifies the frequency of the signal and the length of which is more or less proportional to the intensity of the signal. If the repetitive rate of scanning be made of the order of vfifteen timesa seconder greater, the luminous marks will appear to remain continuously on` thev screen, uctuating inlength as the respective signals uctuate inintensity A lower scanning rate may be employed if desired, however, particularly-if a high'persistence screen I5 be employed.-

The beating oscillators 5 and 9 may be of any type suitable for the functions described. They may comprise electro-mechanical means for cyclically varying the operating frequency or they may be of another Well-known type, commonly employing a voltage-responsive reactance tube. in which the operating frequency is variable under vthe control of an applied voltage. The control voltage applied to oscillator 5`may be a sawtoothed Voltage wave derived from sweep circuit 20 as indicated in Fig. 1. The amplitude of the applied saw-toothed wave determines the extent of the frequency variation of the beating oscillations, and it may be adjusted by means of a variable attenuator 23 or the like. Biasing source 2I of adjustable voltage is interposed to permit adjustment of the mean frequency of the beating oscillations. Attenuator 23 thus controls the extent of the frequency range that is traversed by scanner 3 and the adjustable biasing means 2| determines the absolute frequency position of the portion of the range that is scanned. Switch 25 permitsV disconnection of oscillator 5 from sweep circuit 25 so that if desired scanner 3 may be stopped and adjusted to some particular part of the applied frequency range.

The operating frequency of oscillator 9 is similarly varied in accordance with the amplitude of the control voltage applied to it. Adjustable source 22 allows control of the voltage bias and attenuator 24 controls the extent of variation of the variable applied voltage. In the simplest'case the varying voltage is derived from sweep circuit 2B as indicated in Fig. 1, in which case frequency scanner 'I repeatedly traverses at .a linear rate the pass frequency rangev of filter B in synchronism with the traverse of vscanner 3 across the monitored frequency range. ated, however, that lthe frequency and shape of the periodic wave applied through attenuator 24 determines in general whether the repetitive rate of scanner 'I is the same as or, for example, many times as high as that of scanner 3, and whether scanner 'l operates at a linear rateor in accordance with some other law of variation. Inasmuch as the relative movement of filter I0 across the monitored frequency range is dependent on the combined effect of the voltages used toV control oscillators 5 and 9, it will be appreciated that in the general case both control voltages should jointly influence deflecting plates I 4 if a systematic frequency scale vis to be obtained on screen I5. In the simplest case, however, the two control waves are alike in periodicity and shape and it sumces to connect deflecting plates I4 to the common source, viz., sweep circuit 20.

It may be desired at times to display a small portion of the radio frequency range in considerable detail on the cathode-ray screen I5. Increased detail may be had by adjusting attenuator 24 to reduce the frequency variation of oscillatorY 9, and the frequency range Within which the increased detail is had may be selected by adjustment-of biasing source 22, scanner 3 being stopped at an appropriate point-in the applied frequency range. If desired, too, scanner 'I may be stopped by means of switchv 26'and adjusted manually to select some particular signal. It will be apparent that the several manualcontrols allow considerable flexibility in the operation of the scanningsystem. v

Fig. 3 illustrates Yan embodiment of the invention that utilizes the-'same basic principles as the Fig. 1 system but that is more especially designed for operation over an ultra-highfrequency radio range. Corresponding elements of the several figures, it may be noted, are assigned the same reference numbers. In the interest of a complete disclosure of a specific embodiment of the invention and to facilitate understanding of the construction and operation, specific frequencies and frequency ranges are indicated throughout the Fig. 3 circuit diagram. Thus it will be assumed that the frequency range to be monitored extends from 18 to 80.4 megacycles. All waves within the assumed frequency range are applied through amplifier 2 to the modulator 4 of frequency scanner 3. Beating oscillations for modulator 4 are derived from oscillator 3| which varies in operating frequency from to 35.2 megacycles periodically under the control of sweep circuit 20. A frequency multiplier 32 triples the frequency of the output of oscillator 3|, thus producing oscillations that vary periodically in frequency from 90 to 105.6 megacycles. These oscillations are applied through a band-pass filter to a modulator 33 where they are combined with beating oscillations having a constant frequency of 42 megacycles. The lower side frequency, which ranges from 48 to 63.6 megacycles is applied to a frequency multiplier 34 that doubles the oscillation frequency. The resulting oscillations, which vary periodically between 96 and 127.2 megacycles, are applied then through a filter 35 and buffer amplifier to modulator 4.

In its lower or PI position the upper sideband produced by modulator 4 extends from 114 to 176.4 megacyces, and in its upper or P2 position it extends from 145.2 to 207.6 megacycles, This sideband is applied to scanning filter 6, the passband of which extends from 145.2 to 176.4 megacycles. The relative frequencies are as illustrated in Fig. 2 except that in this case the pass-band of the iilter is half as wide as the applied sideband.

The frequency selection effected by lter 6 is supplemented at another frequency level by filter quency of 400 kilocycles and a pass-band width of kilocycles. Treating filters l0, 39 and 4| with the intervening modulators as a unitary selective means it may be said that the second 2li of the latter system may also be employed for the purposes described.

The tandem-scanning systems herein disclosed have several advantages over comparable singlestage scanning systems of the prior art, and these advantages will be found of considerable im- 1 portance from a practical standpoint in many 31 which is connected to the output of filter. 6

through a frequency transator. The latter comprises a modulator 36 which `is supplied with beating oscillations having a fixed frequency of 115 megacycles and which produces a lower sideband that ranges from 30.2 to 61.4 megacycles, these being the limiting frequencies passed by lter 31.

The wave output of iilter 31 is applied to a second frequency scanner 1 comprising modulator 8' and band-pass filter l0. Modulator 8 receives beating oscillations from filter 35 through a buffer amplifier, thereby producing a 31.2`r`negacycle sideband which in its upper and lower extreme positions extends from 126.2 to 157.4 megacycles and from 157.4 to 188.6 megacycles, respectively. The pass-band of lter l0 extends from about 157.1 to 157.7 megacycles, The frequency selection eifected by filter l0 is supplemented at successively lower frequency levels by filters 39 and 4l which have progressively sharper frequency selective characteristics. larly, the wave output of filter l0 is applied to a modulator 38 which is supplied with beating oscillations having a frequency of 115 megacycles, and the resulting lower sideband is applied to filter 39 which has a pass-band 0.2 megacycle in width ranging downwards from 42.5 megacycles. Modulator 40 receives the 200-kilocycle band from filter 39 and beating oscillations of 42 megacycles. Filter 4I may have a mean pass fre.-

More particuinstances. One advantage lies in the substantial reduction in the frequency change required of the beating oscillations supplied to the modulators. Referring to scanner 3 of the Fig. 1 system,4 the reduction amounts to 25 per cent, for the frequency change required of oscillator 5 is not coextensive with the width of the monitored frequency range but only three-quarters thereof; and in the Fig. 3 system the corresponding reduction is 50 per cent. In scanner 1, likewise, the frequency range covered by the beating oscillations is only a portion of the monitored frequency range. A further advantage lies in the substantial reduction in the ratio of the frequency variation of the beating oscillations to the uppermost beating frequency. 'I'hat is, the practical difficulty of obtaining wide monitoring frequency ranges without resort to high operating frequencies is largely overcome. Still another advantage relates to the scanning, and the production of a magnified view of, only a part of the frequency spectrum for which the system is adapted. In the case of a single-stage scanner this presents the diiculty of providing the beating oscillator with a frequency controller, electrical or mechanical, that is not only operative over the maximum required frequency range but also accurate and sensitive when only a relatively small frequency variation is required. In accordance with the present invention, on the other hand, this difficulty is avoided, for the beating oscillators assoc iated with the successive tandemscanners may be specifically designed for widely different frequency variations and at least one of them may be well adapted for the particular width of frequency range to be scanned and magnified. In`

such case the preceding scanner or scanners may be stopped, as explained hereinbefore.

The specific embodiment illustrated in Fig. 4r

differs from that described with reference to Fig. 3 principally in respect of the means provided for producing the beating oscillations of variable frequency. There are differences also in the frequencies of the fixed oscillators and in the limiting frequencies of the several filters; these frequencies are all indicated in Fig. 4. In the Fig. 4 system there are provided two sweep circuits 20 and 45 that have substantially identical operating frequencies. Theymay be synchronized by connection to a common sine wave source 44 that has a frequency of 15 cycles per second, for specific example. Sweep circuit 20 controls the variable frequency oscillator 3l as described with reference to Figi 3, and sweep circuit 45 controls a'substantially identical oscillator 46. The two sweep circuits 20 and 45 are so biased and poled or otherwise so arranged that the voltage produced bythe one decreases duraiutante'.

7 ing :the period that the voltage .produced by the other increases. Hence theoperating frequency of oscillator 3| progressively increases from 30 to. 35.2 megacycles while that of oscillator 46 progressively decreases from 35.2 to 30 Vmegacycles.

The wave output of oscillator 3| is tripled in frequency by frequency multiplier 32, filtered, and applied to modulator 33 together with beating oscillations having a frequency of .140 megacycles. One of the side frequencies varies from 230 to 245.6 megacycles and this is applied to modulator 45 together with oscillations yof tripled frequency derived from oscillator 46 through frequency .multiplier 4l. The difference frequency, which ranges from 124.4 to 155.6 .megacycles,` is selected by lter 35 and applied to the modulators 4 and 8. Hence during each cycle of the sweep .circuits and 45 the beating oscillations delivered by filter 35 increase progressively from 124.4 to 155.6 megacycles. The variation in beating frequency, that is, 31.2 megacycles, is twice the frequency variation of the oscillations applied to modulator 48.

An important feature of the Fig. 4 system is that any variation in temperature or other operating condition that affects the two Variable frequency oscillators 3l and 46 substantially equally, is largely neutralized in so far as its effect on the frequency cf the oscillations delivered by filter 35 is concerned. For example, a given change in ambient temperature would tend to change the operating frequencies of the two substantially identical oscillators 3l 'and 4B to the same extent and in the same direction. The difference in operating frequency at any instant would remain unaffected, however, and the difference-frequency produced in modulator '48 and supplied through filter 35 to the modulators would likewise be unaffected by the change in temperature.

Although the invention has been described with reference to specific embodiments thereof, it will be understood that the invention may be embodied in various other forms within the spirit and scope of the appended claims.

What is claimed is:

l. In combination, a rst scanner comprising wave translating means for cyclically scanning a predetermined frequency range within which electric waves of different frequencies may ap"- pear, said first scanner including frequency selective means limiting the wave output thereof to a .wave frequency range that is narrower than said first-mentioned frequency range, 'a second scanner connected to receive the said wave output of said rst scanner, said second scanner comprising means for cyclically scanning the said narrower frequency range, said second scanner including frequency selective means limiting the response thereof at any moment to waves within a still narrower frequency range, and means for synchronizing the respective cyclical Aoperations of the first and second scanners.

2. A combination in accordance with claim Y1 in which said last-mentioned frequency selective means is at least several times more sharply selective than the first-mentioned frequency selective means.

v3. AA wave frequency 'range scanning system comprising a modulator, said modulator having electric wave input means, a pair of substantially identical oscillation generators, means 'for varying the oscillation frequency Vof said 'generator cyclical-ly, in mutually opposite senses, `and to substantially the same extent, means for deriving 'from said oscillation generators a bea-ting oscillation the frequency of which cyclically varies as a function of the difference between said oscillation frequencies, means for supplying said beating oscillations to said modulator, and frequency selective means connected to receive modulation products from said modulatorJ 4. In combination, a pair of oscillation generating means, .means for varying the respective oscillation frequencies of said generating means lcyclically and in mutually opposite senses between substantially the same predetermined frequency limits, means for deriving from the oscillations generated by said pair of means a beating oscillation, the frequency of which var-ies cyclically-as a function of the difference between said oscillation frequencies, a modulator, means for applying waves to said modulator, means for concurrently applying said beating oscillation to said modulator, frequency selective wave transmission means having a transmission band that is substantially smaller than the frequency interval over which the frequency of said beating oscillation varies, said transmission means being connected to receive the wave output of said modulator, an oscilloscope having a luminescent screen and means for directing a luminescenceproducing ray to said screen, means for deflecting said ray repeatedly across said screen in timed relation with the variation in frequency of said beating oscillation, and means for variably con' trolling said ray responsive to variations in the wave output of said frequency selective wave transmission means.

5. In combination, in a wave frequency range scanning system, an electric wave transmission path including in the relative order named, a first modulator, a rst filter, a second modulator and a second lter, means for supplying to each of said modulators beating oscillations the frequency of which varies cyclically between predetermined limits, each of said filters having a transmission band not substantially wider than the range of frequency variation of the beating oscillations supplied to the modulator next preceding i-t, the transmission band of said rst fil'- ter being at least several times as wide as the transmission band of said second filter, and means for synchronizing the respective cyclical variations of said beating oscillations supplied to said modulators.

6. .In a Wave frequency range scanningv system comprising an electric wave transmission path including in the relative order named, an electric Wave input device, a first modulator, a first filter, a-second modulator and a second filter, means for supplying to each of said modulators beating oscillations the frequency of which varies cyclically between predetermined limits, means for synchronizing the respective cyclical variations of .said beating oscillations supplied to said modulators, each of said filters having a transmission band not substantially wider than the range of frequency variation of the beating oscillations supplied to the modulator next preceding it, whereby input electric waves occupying a predetermined frequency band are scanned, the transmission band of said first filter being at least several times as wide as the transmission band of said second filter and being centered at a frequency that is greater than the width of said predetermined frequency band.

'7. In combination, in a wave receiving system,

a first modulator, means for impressing received waves on said modulator, means for concurrently impressing on said modulator beating oscillations the frequency of which varies cyclically over a first frequency interval, a first band-pass filter means connected to pass waves of the upper sideband only from the output of said modulator, a second modulator, wave translating means for impressing the wave output of said rst filter means on said second modulator. means for concurrently impressing on said second modulator beating oscillations the frequency of which varies cyclically over a second frequency interval, means for synchronizing the respective cyclical variations of said beating oscillations supplied to said modulators, a second band-pass lter means connected to receive the wave output of said second modulator, utilization means connected to receive the wave output of said second filter means, said first frequency interval being at least substantially double the bandwidth of said first filter means, and both said second frequency interval and the said bandwidth of said first filter means being at least several times the band-width of said second filter means, said utilization means including a cathode ray oscilloscope, means for deiiecting the cathode ray in predetermined correlation with the frequency variations of the beating oscillations impressed on said modulators, and ray controlling means continually responsive to the wave output of said second lter means.

EDMUND R. TAYLOR.

10 REFERENCES CITED The following references are of record in the file of this patent:

UNITED STATES PATENTS Number Name Date 1,753,444 Ohl Apr. 8, 1930 1,866,267 Nicolson July 5, 1932 1,882,772 Callahan Oct. 18, 1932 1,883,907 Hathaway Oct. 25, 1932 1,994,232 Schuck, Jr Mar. 12, 1935 2,121,359 Luck et al. June 21, 1938 2,178,074 Jakel et al Oct. 31, 1939 2,240,452 Wolfskill Apr. 29, 1941 2,279,151 Wallace Apr. 7, 1942 2,279,246 Podliasky et al Apr. 7, 1942 2,282,092 Roberts May 5, 1942 2,287,925 White June 30, 1942 2,302,311 Goldsmith Nov. 17, 1942 2,307,029 Elm Jan. 5, 1943 2,333,322 Levy Nov. 2, 1943 2,343,115 Noble Feb. 29, 1944 2,361,956 Moseley Nov. 7, 1944 2,381,940 Wallace et al Aug. 14, 1945 2,387,685 Sanders Oct. 23, 1945 2,416,346 Potter Feb. 25, 1947 2,445,562 Cawein et al. July 20, 1948 2,502,294 Wallace Mar. 28, 1950 FOREIGN PATENTS Number Country VDate 687,771 France Jan. 7, 1930

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